JP2020053486A - Inductor - Google Patents

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JP2020053486A
JP2020053486A JP2018179301A JP2018179301A JP2020053486A JP 2020053486 A JP2020053486 A JP 2020053486A JP 2018179301 A JP2018179301 A JP 2018179301A JP 2018179301 A JP2018179301 A JP 2018179301A JP 2020053486 A JP2020053486 A JP 2020053486A
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magnetic layer
laminated
laminated portion
magnetic
core
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正剛 白井
Masatake Shirai
正剛 白井
佐藤 嘉千安
Kachiyasu Sato
嘉千安 佐藤
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Murata Manufacturing Co Ltd
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Priority to JP2018179301A priority Critical patent/JP2020053486A/en
Priority to CN201910851943.8A priority patent/CN110942883A/en
Priority to US16/577,223 priority patent/US11430603B2/en
Publication of JP2020053486A publication Critical patent/JP2020053486A/en
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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F27/00Details of transformers or inductances, in general
    • H01F27/28Coils; Windings; Conductive connections
    • H01F27/30Fastening or clamping coils, windings, or parts thereof together; Fastening or mounting coils or windings on core, casing, or other support
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F27/00Details of transformers or inductances, in general
    • H01F27/24Magnetic cores
    • H01F27/245Magnetic cores made from sheets, e.g. grain-oriented
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F17/00Fixed inductances of the signal type 
    • H01F17/04Fixed inductances of the signal type  with magnetic core
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F27/00Details of transformers or inductances, in general
    • H01F27/24Magnetic cores
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F27/00Details of transformers or inductances, in general
    • H01F27/24Magnetic cores
    • H01F27/26Fastening parts of the core together; Fastening or mounting the core on casing or support
    • H01F27/263Fastening parts of the core together
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F27/00Details of transformers or inductances, in general
    • H01F27/28Coils; Windings; Conductive connections
    • H01F27/2823Wires
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F27/00Details of transformers or inductances, in general
    • H01F27/28Coils; Windings; Conductive connections
    • H01F27/2823Wires
    • H01F27/2828Construction of conductive connections, of leads
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F27/00Details of transformers or inductances, in general
    • H01F27/28Coils; Windings; Conductive connections
    • H01F27/2847Sheets; Strips
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F27/00Details of transformers or inductances, in general
    • H01F27/34Special means for preventing or reducing unwanted electric or magnetic effects, e.g. no-load losses, reactive currents, harmonics, oscillations, leakage fields
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F3/00Cores, Yokes, or armatures
    • H01F3/10Composite arrangements of magnetic circuits
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F3/00Cores, Yokes, or armatures
    • H01F3/10Composite arrangements of magnetic circuits
    • H01F2003/106Magnetic circuits using combinations of different magnetic materials
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F17/00Fixed inductances of the signal type 
    • H01F17/04Fixed inductances of the signal type  with magnetic core
    • H01F2017/048Fixed inductances of the signal type  with magnetic core with encapsulating core, e.g. made of resin and magnetic powder
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F27/00Details of transformers or inductances, in general
    • H01F27/34Special means for preventing or reducing unwanted electric or magnetic effects, e.g. no-load losses, reactive currents, harmonics, oscillations, leakage fields
    • H01F2027/348Preventing eddy currents

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  • Engineering & Computer Science (AREA)
  • Power Engineering (AREA)
  • Microelectronics & Electronic Packaging (AREA)
  • Chemical & Material Sciences (AREA)
  • Composite Materials (AREA)
  • Coils Or Transformers For Communication (AREA)
  • Manufacturing Cores, Coils, And Magnets (AREA)

Abstract

To provide an inductor in which eddy current loss is reduced.SOLUTION: An inductor 100 comprises a core 30a including lamination parts 31a-33a where magnetic layers 41a, 42a and isolating layers 51a, 52a are laminated alternately, a coil 20 including a wound part 21 wound around the core 30a, the reel of the wound part 21 being placed substantially orthogonally to the lamination direction, and an element 40 receiving the core 30a and the coil 20. The lamination parts 31a-33a include a first lamination part 31a where the first magnetic layer 41a and the isolating layer 51a are laminated alternately, and a second lamination part 32a and a third lamination part 33a where the second magnetic layer and the isolating layer are laminated alternately. The first lamination part 31a has first and second faces orthogonal to the lamination direction and facing each other, and third and fourth faces parallel with the lamination direction and the reel direction and facing each other. The second lamination part 32a is placed on the first face, and the third lamination part 33a is placed on the second face.SELECTED DRAWING: Figure 1

Description

本発明は、インダクタに関する。   The present invention relates to inductors.

DCDCコンバータ等のチョークコイルに用いられるパワーインダクタとして、軟磁性合金からなる磁性粉末と樹脂とを混練した封止材でコイルを封止したインダクタが広く利用されている。例えば、特許文献1に記載されるインダクタは、加圧成形した封止材でコイルを挟み、さらに加圧することによって成形されて製造される。   As a power inductor used for a choke coil of a DCDC converter or the like, an inductor in which a coil is sealed with a sealing material obtained by kneading a magnetic powder made of a soft magnetic alloy and a resin is widely used. For example, the inductor described in Patent Literature 1 is manufactured by forming a coil by sandwiching a coil with a pressure-molded sealing material and further pressing the coil.

特開2016−119385号公報JP-A-2006-193385 国際公開第2018/079402号WO2018 / 079402

上記のような封止材は、軟磁性合金からなる磁性粉末と樹脂とを混練したものなので、封止材中の磁性粉の占める割合が低いので比透磁率が低い。そのため、封止材でコイルを封止したインダクタは、単一の軟磁性合金等からなるインダクタに比べて、インダクタンス値を高くできない。所望のインダクタンス値を得るためには、コイルの巻回数を多くする必要があり、インダクタの直流抵抗が高くなり易いという問題があった。このような問題を解決するため、特許文献2には、軟磁性体層と絶縁体層が交互に積層されたコアをコイルの内部空有間に配置するインダクタが開示されている。特許文献2に記載されたインダクタは、コイルの巻回数を多くしなくても所望のインダクタンス値を得られ、コイルに流れる電流により磁場で発生する渦電流損失等を低減することができる。しかしながら、DCDCコンバータの高効率化のため、さらに渦電流損失を低減する必要がある。   Since the above-mentioned sealing material is obtained by kneading a magnetic powder made of a soft magnetic alloy and a resin, the ratio of the magnetic powder in the sealing material is low, so that the relative permeability is low. Therefore, the inductor whose coil is sealed with the sealing material cannot have a higher inductance value than an inductor made of a single soft magnetic alloy or the like. In order to obtain a desired inductance value, it is necessary to increase the number of turns of the coil, and there is a problem that the DC resistance of the inductor tends to increase. In order to solve such a problem, Patent Literature 2 discloses an inductor in which a core in which soft magnetic layers and insulating layers are alternately stacked is disposed between the internal spaces of a coil. The inductor described in Patent Literature 2 can obtain a desired inductance value without increasing the number of turns of the coil, and can reduce eddy current loss and the like generated by a magnetic field due to a current flowing through the coil. However, in order to increase the efficiency of the DCDC converter, it is necessary to further reduce the eddy current loss.

本発明は、上記の課題を鑑み、コアを有しながら、渦電流損失が低減されるインダクタの提供を目的とする。   The present invention has been made in view of the above problems, and has as its object to provide an inductor having a core and reduced eddy current loss.

本発明のインダクタの一態様は、磁性層と絶縁層とが交互に積層される積層部を含むコアと、コアの周囲に巻回される巻回部と巻回部から引き出される1対の引き出し部を含み、巻回部の巻軸が積層部の積層方向と略直交して配置されるコイルと、対向する端面を有し、コアおよびコイルを収容する素体とを備える。磁性層は、第1磁性層と、第1磁性層よりも電気抵抗率が大きい第2磁性層とを含む。積層部は、第1磁性層および絶縁層が交互に積層される第1積層部と、第2磁性層および絶縁層が交互に積層される第2積層部および第3積層部とを含む。第1積層部は、積層方向に直交し、互いに対向する第1の面および第2の面と、積層方向および巻軸方向に平行な面であり、互いに対向する第3の面および第4の面とを有する。第2積層部は第1の面に配置され、第3積層部は第2の面に配置されるか、または、第2積層部は第3の面に配置され、第3積層部は第4の面に配置される。   One embodiment of the inductor of the present invention is a core including a laminated portion in which a magnetic layer and an insulating layer are alternately laminated, a wound portion wound around the core, and a pair of drawers pulled out from the wound portion. And a coil in which the winding axis of the winding portion is disposed substantially perpendicular to the laminating direction of the laminating portion, and a body having an end face facing the housing and accommodating the core and the coil. The magnetic layer includes a first magnetic layer and a second magnetic layer having a higher electrical resistivity than the first magnetic layer. The stacked unit includes a first stacked unit in which first magnetic layers and insulating layers are alternately stacked, and a second stacked unit and third stacked units in which second magnetic layers and insulating layers are alternately stacked. The first laminated portion is a first surface and a second surface that are orthogonal to the laminating direction and oppose each other, and a third surface and a fourth surface that are parallel to the laminating direction and the winding axis direction. Surface. The second laminated portion is disposed on the first surface, the third laminated portion is disposed on the second surface, or the second laminated portion is disposed on the third surface, and the third laminated portion is disposed on the fourth surface. Placed on the surface.

本発明のインダクタの一態様は、磁性層と絶縁層とが交互に積層される積層部を含むコアと、コアの周囲に巻回される巻回部と巻回部から引き出される1対の引き出し部を含み、巻回部の巻軸が積層部の積層方向と略直交して配置されるコイルと、対抗する端面を有し、コアおよびコイルを収容する素体とを備える。磁性層は、第1磁性層と、第1磁性層よりも比透磁率が大きい第2磁性層とを含む。積層部は、第1磁性層および絶縁層が交互に積層される第1積層部と、第2磁性層および絶縁層が交互に積層される第2積層部および第3積層部とを含む。第1積層部は、積層方向に直交し、互いに対向する第1の面および第2の面と、積層方向および巻軸方向に平行な面であり、互いに対向する第3の面および第4の面とを有する。第2積層部は第1の面に配置され、第3積層部は第2の面に配置されるか、または、第2積層部は第3の面に配置され、第3積層部は第4の面に配置される。   One embodiment of the inductor of the present invention is a core including a laminated portion in which magnetic layers and insulating layers are alternately laminated, a wound portion wound around the core, and a pair of drawers drawn out from the wound portion. And a coil in which the winding axis of the winding portion is disposed substantially perpendicular to the laminating direction of the laminating portion, and a body having opposing end faces and accommodating the core and the coil. The magnetic layer includes a first magnetic layer and a second magnetic layer having a higher relative magnetic permeability than the first magnetic layer. The stacked unit includes a first stacked unit in which first magnetic layers and insulating layers are alternately stacked, and a second stacked unit and third stacked units in which second magnetic layers and insulating layers are alternately stacked. The first laminated portion is a first surface and a second surface that are orthogonal to the laminating direction and oppose each other, and a third surface and a fourth surface that are parallel to the laminating direction and the winding axis direction. Surface. The second laminated portion is disposed on the first surface, the third laminated portion is disposed on the second surface, or the second laminated portion is disposed on the third surface, and the third laminated portion is disposed on the fourth surface. Placed on the surface.

本発明によれば、コアを有しながら、渦電流損失が低減されるインダクタを提供することができる。   According to the present invention, it is possible to provide an inductor in which eddy current loss is reduced while having a core.

実施例1のインダクタの概略透過斜視図である。FIG. 2 is a schematic transparent perspective view of the inductor according to the first embodiment. 図1のインダクタの概略断面図である。FIG. 2 is a schematic sectional view of the inductor of FIG. 1. 実施例4のインダクタのコアの一例を示す概略斜視図である。FIG. 14 is a schematic perspective view illustrating an example of a core of an inductor according to a fourth embodiment. 実施例5のインダクタの概略断面図である。FIG. 13 is a schematic sectional view of an inductor according to a fifth embodiment. 実施例6のインダクタのコアの一例を示す概略斜視図である。FIG. 14 is a schematic perspective view illustrating an example of a core of an inductor according to a sixth embodiment. 実施例7のインダクタのコアの一例を示す概略斜視図である。FIG. 16 is a schematic perspective view illustrating an example of a core of an inductor according to a seventh embodiment. 実施例8のインダクタのコアの一例を示す概略斜視図である。FIG. 21 is a schematic perspective view illustrating an example of a core of an inductor according to an eighth embodiment.

本実施形態に係るインダクタは、磁性層と絶縁層とが交互に積層される積層部を含むコアと、コアの周囲に巻回される巻回部と巻回部から引き出される1対の引き出し部を含むコイルと、対向する端面を有し、コアおよび前記コイルを収容する素体とを備える。コイルは巻回部の巻軸を積層部の積層方向と略直交させて配置される。また、磁性層は、第1磁性層と、第1磁性層よりも電気抵抗率が大きい第2磁性層とを含む。積層部は、第1磁性層および絶縁層が交互に積層される第1積層部と、第2磁性層および絶縁層が交互に積層される第2積層部および第3積層部とを含む。第1積層部は、積層方向に直交し、互いに対向する第1の面および第2の面と、積層方向および巻軸方向に平行な面であり、互いに対向する第3の面および第4の面とを有する。第2積層部は前記第1の面に配置され、第3積層部は第2の面に配置されるか、または、第2積層部は第3の面に配置され、第3積層部は前記第4の面に配置される。   The inductor according to the present embodiment includes a core including a laminated portion in which a magnetic layer and an insulating layer are alternately laminated, a wound portion wound around the core, and a pair of lead portions pulled out from the wound portion. And a body having an end surface facing the core and accommodating the core and the coil. The coil is arranged so that the winding axis of the winding portion is substantially perpendicular to the lamination direction of the lamination portion. Further, the magnetic layer includes a first magnetic layer and a second magnetic layer having a higher electric resistivity than the first magnetic layer. The stacked unit includes a first stacked unit in which first magnetic layers and insulating layers are alternately stacked, and a second stacked unit and third stacked units in which second magnetic layers and insulating layers are alternately stacked. The first laminated portion is a first surface and a second surface that are orthogonal to the laminating direction and oppose each other, and a third surface and a fourth surface that are parallel to the laminating direction and the winding axis direction. Surface. The second laminated portion is disposed on the first surface, the third laminated portion is disposed on the second surface, or the second laminated portion is disposed on the third surface, and the third laminated portion is disposed on the third surface. It is arranged on the fourth surface.

インダクタでは、コアが磁性層と絶縁層とを積層してなる積層部から形成され、積層部の積層方向すなわち磁性層の厚み方向をコイルの巻回部の巻軸に略直交させて、巻回部の内部空間に配置されている。積層部では、第1磁性層よりも電気抵抗率が大きい第2磁性層から形成される第2積層部および第3積層部が、第2磁性層よりも電気抵抗率が小さい第1磁性層から形成される第1積層部の外側面上に配置され、巻回部の導線に近接している。第2積層部および第3積層部では第2磁性層の電気抵抗率が大きいため、磁路に直交する磁性層の断面で発生する渦電流が小さくなり、電気抵抗率が小さい第1磁性層をコイルの巻回部に近接して配置する場合よりも渦電流損失を低減することができる。これにより、特にインダクタがDCDCコンバータのチョークコイルに用いられた場合のDCDCコンバータの軽負荷時において、磁束が通過する第2積層部および第3積層部における渦電流損失が低減されることになる。   In the inductor, the core is formed of a laminated portion formed by laminating a magnetic layer and an insulating layer, and the laminating direction of the laminated portion, that is, the thickness direction of the magnetic layer is substantially orthogonal to the winding axis of the winding portion of the coil. It is arranged in the internal space of the unit. In the laminated portion, the second laminated portion and the third laminated portion formed from the second magnetic layer having a higher electric resistivity than the first magnetic layer are separated from the first magnetic layer having a lower electric resistivity than the second magnetic layer. It is arrange | positioned on the outer surface of the 1st laminated part formed, and is close to the conductor of a winding part. In the second laminated portion and the third laminated portion, since the electric resistivity of the second magnetic layer is large, the eddy current generated in the cross section of the magnetic layer orthogonal to the magnetic path is reduced, and the first magnetic layer having the small electric resistivity is reduced. The eddy current loss can be reduced as compared with the case where the coil is arranged close to the winding part of the coil. This reduces the eddy current loss in the second and third laminated portions through which the magnetic flux passes, especially when the DCDC converter is under a light load when the inductor is used in the choke coil of the DCDC converter.

インダクタは、磁性層と絶縁層とが交互に積層される積層部を含むコアと、コアの周囲に巻回される巻回部と巻回部から引き出される1対の引き出し部を含むコイルと、対向する端面を有し、コアおよび前記コイルを収容する素体とを備える。コイルは巻回部の巻軸を積層部の積層方向と略直交させて配置される。また、磁性層は、第1磁性層と、第1磁性層よりも比透磁率が大きい第2磁性層とを含む。積層部は、第1磁性層および絶縁層が交互に積層される第1積層部と、第2磁性層および絶縁層が交互に積層される第2積層部および第3積層部とを含む。第1積層部は、積層方向に直交し、互いに対向する第1の面および第2の面と、積層方向および巻軸方向に平行な面であり、互いに対向する第3の面および第4の面とを有する。第2積層部は第1の面に配置され、第3積層部は第2の面に配置されるか、または、第2積層部は第3の面に配置され、第3積層部は第4の面に配置される。第2積層部および第3積層部では第2磁性層の比透磁率が大きいため、磁路に直交する磁性層の断面で発生する渦電流が小さくなり、比透磁率が小さい第1磁性層をコイルの巻回部に近接して配置する場合よりも渦電流損失を低減することができる。   An inductor includes a core including a laminated portion in which a magnetic layer and an insulating layer are alternately laminated, a coil including a wound portion wound around the core and a pair of lead portions pulled out from the wound portion, A core having a core and the coil; The coil is arranged so that the winding axis of the winding portion is substantially perpendicular to the lamination direction of the lamination portion. The magnetic layer includes a first magnetic layer and a second magnetic layer having a higher relative magnetic permeability than the first magnetic layer. The stacked unit includes a first stacked unit in which first magnetic layers and insulating layers are alternately stacked, and a second stacked unit and third stacked units in which second magnetic layers and insulating layers are alternately stacked. The first laminated portion is a first surface and a second surface that are orthogonal to the laminating direction and oppose each other, and a third surface and a fourth surface that are parallel to the laminating direction and the winding axis direction. Surface. The second laminated portion is disposed on the first surface, the third laminated portion is disposed on the second surface, or the second laminated portion is disposed on the third surface, and the third laminated portion is disposed on the fourth surface. Placed on the surface. Since the relative permeability of the second magnetic layer is large in the second laminated portion and the third laminated portion, the eddy current generated in the cross section of the magnetic layer orthogonal to the magnetic path is reduced, and the first magnetic layer having a small relative permeability is reduced. The eddy current loss can be reduced as compared with the case where the coil is arranged close to the winding part of the coil.

インダクタの積層部では、第2磁性層の電気抵抗率と比透磁率との積は、第1磁性層の電気抵抗率と比透磁率との積よりも大きくなっていてもよい。これにより、インダクタに流れる直流重畳電流が小さい軽負荷時におけるインダクタに生じる渦電流損失を低減することができる。   In the laminated portion of the inductor, the product of the electric resistivity of the second magnetic layer and the relative magnetic permeability may be larger than the product of the electric resistivity of the first magnetic layer and the relative magnetic permeability. As a result, eddy current loss that occurs in the inductor at a light load when the DC superimposed current flowing through the inductor is small can be reduced.

インダクタでは、1対の引き出し部が、巻回部の外周から素体の対向する端面方向にそれぞれ引き出されており、端面と平行な断面において、引き出し部が引き出される側の巻回部のコイル巻数は、引き出し部が引き出される側に対向する側よりも1ターン多くなっているので、第2積層部における第2磁性層の積層数と、第3積層部における第2磁性層の積層数とが異なっていてもよい。1対の引き出し部は、巻回部の外周から素体の対向する端面方向にそれぞれ逆向きに引き出される場合、一方の引き出し部側に配置される第2積層部または第3積層部における第2磁性層の積層数を多くすることで、より効果的に軽負荷時における渦電流損失を低減することができる。   In the inductor, a pair of lead portions is pulled out from the outer periphery of the winding portion in the direction of the facing end surface of the element body, and in a cross section parallel to the end surface, the number of coil turns of the winding portion on the side from which the drawing portion is pulled out. Is one turn more than the side opposite to the side from which the drawer is pulled out, so that the number of laminations of the second magnetic layer in the second lamination and the number of lamination of the second magnetic layer in the third lamination are It may be different. When the pair of lead portions are pulled out from the outer periphery of the winding portion in the opposite end surface directions of the element body in the opposite directions, the second stacked portion or the second stacked portion disposed on one of the drawn portion sides By increasing the number of stacked magnetic layers, the eddy current loss under light load can be reduced more effectively.

第1積層部、第2積層部および第3積層部のうち、少なくとも2つの積層方向が異なっていてもよい。例えば、第2積層部および第3積層部の積層方向と、第1積層部の積層方向とを、例えば、略直交させて配置することで、より効果的に軽負荷時における渦電流損失を低減することができる。   At least two of the first stacked unit, the second stacked unit, and the third stacked unit may have different stacking directions. For example, by arranging the lamination direction of the second and third lamination portions and the lamination direction of the first lamination portion substantially at right angles, for example, eddy current loss at light load can be more effectively reduced. can do.

第1積層部、第2積層部および第3積層部のうち、少なくとも1つの積層部は巻回部の巻軸方向に直交する少なくとも1つの面で分割されていてもよい。例えば、第2積層部および第3積層部のうち、少なくとも1つの積層部を巻回部の巻軸方向に直交する少なくとも1つの面で分割することで、より効果的に軽負荷時における渦電流損失を低減することができる。   At least one of the first stacked unit, the second stacked unit, and the third stacked unit may be divided by at least one surface orthogonal to the winding axis direction of the winding unit. For example, by dividing at least one of the second laminated portion and the third laminated portion by at least one surface orthogonal to the direction of the winding axis of the winding portion, the eddy current at light load can be more effectively achieved. Loss can be reduced.

第1磁性層の厚みと第2磁性層の厚みとが異なっていてもよい。その場合、コアにおいては、第2磁性層の厚みの二乗を第2磁性層の比透磁率と電気抵抗率の積の平方根で除した数値が、第1磁性層の厚みの二乗を第1磁性層の比透磁率と電気抵抗率の積の平方根で除した数値よりも小さくなっていてもよい。渦電流損失は、磁性層の厚みの二乗に比例し、磁性層の比透磁率と電気抵抗率の積の平方根に反比例するため、上記関係を満たすことで、より効果的に軽負荷時における渦電流損失を低減することができる。   The thickness of the first magnetic layer and the thickness of the second magnetic layer may be different. In this case, in the core, a value obtained by dividing the square of the thickness of the second magnetic layer by the square root of the product of the relative magnetic permeability and the electric resistivity of the second magnetic layer is obtained by dividing the square of the thickness of the first magnetic layer by the first magnetic layer. It may be smaller than a value obtained by dividing by the square root of the product of the relative magnetic permeability and the electric resistivity of the layer. The eddy current loss is proportional to the square of the thickness of the magnetic layer, and is inversely proportional to the square root of the product of the relative magnetic permeability and the electric resistivity of the magnetic layer. Current loss can be reduced.

以下、本発明の実施形態を図面に基づいて説明する。ただし、以下に示す実施形態は、本発明の技術思想を具体化するための、インダクタを例示するものであって、本発明は、以下に示すインダクタに限定されない。なお、特許請求の範囲に示される部材を、実施形態の部材に限定するものでは決してない。特に、実施形態に記載されている構成部品の寸法、材質、形状、その相対的配置等は特に特定的な記載がない限りは、本発明の範囲をそれのみに限定する趣旨ではなく、単なる説明例にすぎない。なお、各図面が示す部材の大きさ、位置関係等は、説明を明確にするため誇張していることがある。さらに、以下の説明において、同一の名称、符号については同一もしくは同質の部材を示しており、詳細説明を適宜省略する。またさらに、本発明を構成する各要素は、複数の要素を同一の部材で構成して一の部材で複数の要素を兼用する態様としてもよいし、逆に一の部材の機能を複数の部材で分担して実現することもできる。また、一部の実施例において説明された内容は、他の実施例に利用可能なものもある。実施例2以降では実施例1と共通の事柄についての記述を省略し、異なる点についてのみ説明する。特に、同様の構成による同様の作用効果については実施形態毎には逐次言及しない。   Hereinafter, embodiments of the present invention will be described with reference to the drawings. However, the embodiment described below exemplifies an inductor for embodying the technical idea of the present invention, and the present invention is not limited to the inductor described below. Note that the members described in the claims are not limited to the members of the embodiment. In particular, the dimensions, materials, shapes, relative arrangements, and the like of the components described in the embodiments are not intended to limit the scope of the present invention thereto, unless otherwise specified. It is only an example. In addition, the size, positional relationship, and the like of the members illustrated in each drawing may be exaggerated for clarity of description. Further, in the following description, the same names and reference numerals denote the same or similar members, and a detailed description thereof will be appropriately omitted. Still further, each element constituting the present invention may be configured such that a plurality of elements are formed of the same member and one member also serves as the plurality of elements, or conversely, the function of one member may be a plurality of members. It can also be realized by sharing. In addition, the contents described in some embodiments can be used in other embodiments. In the second and subsequent embodiments, description of matters common to the first embodiment will be omitted, and only different points will be described. In particular, the same operation and effect of the same configuration will not be sequentially described for each embodiment.

(実施例1)
実施例1のインダクタ100を図1および図2を参照して説明する。図1はインダクタ100の一例を示す概略透過斜視図である。図2は、図1のA−A線を通り、コイルの巻軸に平行な面におけるインダクタ100の概略断面図である。
(Example 1)
First Embodiment An inductor 100 according to a first embodiment will be described with reference to FIGS. FIG. 1 is a schematic transparent perspective view showing an example of the inductor 100. FIG. 2 is a schematic cross-sectional view of inductor 100 taken along a line AA in FIG. 1 and parallel to the winding axis of the coil.

図1に示すように、インダクタ100は、巻回部21と巻回部21から引き出される1対の引き出し部22aおよび22bからなるコイル20と、コイル20の巻回部21に包囲されるコア30aと、コイル20およびコア30aを収容する素体40と、引き出し部22aおよび22bにそれぞれ電気的に接続する1対の外部端子60とを備える。巻回部21の巻軸方向Zからみた外周形状は、長軸および短軸を有する楕円形状または長円形状である。素体40は、実装面側の底面と、底面に対向する上面と、底面および上面に隣接し、互いに対向する1対の端面70および1対の側面72とを有する。1対の端面70は巻回部21の長軸方向と略直交し、1対の側面72は巻回部21の短軸方向と略直交する。また、素体40は巻回部21の巻軸に直交する断面における長軸方向に平行な長手方向Lと、巻回部21の長軸方向に直交する短軸方向に平行な短手方向Wと、巻軸方向Zに平行な素体の高さ方向Hを有する。   As shown in FIG. 1, the inductor 100 includes a coil 20 including a winding part 21 and a pair of lead parts 22 a and 22 b drawn from the winding part 21, and a core 30 a surrounded by the winding part 21 of the coil 20. And a body 40 accommodating the coil 20 and the core 30a, and a pair of external terminals 60 electrically connected to the lead portions 22a and 22b, respectively. The outer peripheral shape of the winding portion 21 as viewed from the winding axis direction Z is an elliptical shape having a major axis and a minor axis or an elliptical shape. The element body 40 has a bottom surface on the mounting surface side, a top surface facing the bottom surface, and a pair of end surfaces 70 and a pair of side surfaces 72 adjacent to the bottom surface and the top surface and facing each other. The pair of end surfaces 70 are substantially orthogonal to the long axis direction of the winding portion 21, and the pair of side surfaces 72 are substantially orthogonal to the short axis direction of the winding portion 21. The element body 40 has a longitudinal direction L parallel to the long axis direction in a cross section orthogonal to the winding axis of the winding portion 21 and a short direction W parallel to the short axis direction orthogonal to the long axis direction of the winding portion 21. And a height direction H of the body parallel to the winding axis direction Z.

素体40は、コイル20とコア30aが埋設された複合材料に圧力をかけて形成される。素体40を形成する複合材料は、例えば、磁性粉と樹脂等の結着剤とを含む。磁性粉には、例えば、鉄(Fe)、Fe−Si系、Fe−Si−Cr系、Fe−Si−Al系、Fe−Ni−Al系、Fe−Cr−Al系等の鉄系の金属磁性粉、鉄を含まない組成系の金属磁性粉、鉄を含む他の組成系の金属磁性粉、アモルファス状態の金属磁性粉、表面がガラス等の絶縁体で被覆された金属磁性粉、表面を改質した金属磁性粉、ナノ結晶状態の金属磁性粉、多結晶状態の金属磁性粉、フェライト粉等を用いることができる。また、結着剤には、エポキシ樹脂、ポリイミド樹脂、フェノール樹脂等の熱硬化性樹脂、ポリエステル樹脂、ポリアミド樹脂等の熱可塑性樹脂が用いられる。   The element body 40 is formed by applying pressure to the composite material in which the coil 20 and the core 30a are embedded. The composite material forming the element body 40 includes, for example, a magnetic powder and a binder such as a resin. Examples of the magnetic powder include iron-based metals such as iron (Fe), Fe-Si, Fe-Si-Cr, Fe-Si-Al, Fe-Ni-Al, and Fe-Cr-Al. Magnetic powder, metal magnetic powder of a composition not containing iron, metal magnetic powder of another composition containing iron, metal magnetic powder in an amorphous state, metal magnetic powder whose surface is covered with an insulator such as glass, Modified metallic magnetic powder, nanocrystalline metallic magnetic powder, polycrystalline metallic magnetic powder, ferrite powder and the like can be used. Further, as the binder, a thermosetting resin such as an epoxy resin, a polyimide resin, and a phenol resin, and a thermoplastic resin such as a polyester resin and a polyamide resin are used.

コイル20は、絶縁被覆を有する断面矩形の導線(以下、平角線ともいう)を、引き出し部22aおよび22bが外周に位置し、巻回部21が渦巻き状の2段に巻き回されて形成されている。巻回部21は、導線が巻回される巻回部21の内側にコア30aを収納する空間を有し、巻軸を素体40の底面および上面に略直交させて素体40の内部に配置されている。1対の引き出し部22aおよび22bは、巻回部の最外周から互いに反対方向に素体40の長手方向Lの端面70方向に向けてそれぞれ引き出され、素体40のそれぞれの端面70から引き出し部22aおよび22bの一部が露出している。素体40の端面70および底面の一部には、素体40から露出する引き出し部22aおよび22bに電気的に接続する外部端子60がそれぞれ設けられる。   The coil 20 is formed by winding a conducting wire having a rectangular cross section (hereinafter, also referred to as a flat wire) having an insulating coating, with the lead portions 22a and 22b positioned on the outer periphery and the winding portion 21 wound in two spiral steps. ing. The winding part 21 has a space for accommodating the core 30 a inside the winding part 21 around which the conductive wire is wound, and the winding axis is substantially orthogonal to the bottom surface and the top surface of the element body 40, and Are located. The pair of lead portions 22a and 22b are pulled out from the outermost periphery of the winding portion in opposite directions toward the end face 70 in the longitudinal direction L of the body 40, and are drawn out from the respective end faces 70 of the body 40. Parts of 22a and 22b are exposed. External terminals 60 that are electrically connected to the lead portions 22a and 22b exposed from the element body 40 are provided on the end face 70 and a part of the bottom surface of the element body 40, respectively.

コア30aは、第1磁性層41aと絶縁層51aとが交互に積層される第1積層部31aと、厚みおよび比透磁率が第1磁性層と等しく、電気抵抗率が第1磁性層より大きい第2磁性層42aと絶縁層52aとが交互に積層される第2積層部32aおよび第2磁性層42aと絶縁層53aとが交互に積層される第3積層部33aとを備える。第1積層部31a、第2積層部32aおよび第3積層部33a(併せて、単に積層部ともいう)は、それぞれが直方体形状を有している。また、第1積層部31aは、積層方向に直交して最外層に位置して、互いに対向する第1の面および第2の面と、第1の面および第2の面に隣接し、積層方向および巻軸方向に平行な面であり、互いに対向する第3の面および第4の面と、それら以外の2つの側面とを有する。インダクタ100では、第2積層部32a、第1積層部31aおよび第3積層部33aは、積層方向を一致させてこの順に積層されてコア30aを形成している。すなわち、第2積層部32aおよび第3積層部33aは、それぞれ第1積層部31aの互いに対向する第1の面と第2の面上に、積層方向が平行になるように配置される。コア30aは積層方向を、巻回部21の巻軸と略直交させて巻回部21の内部空間に収容される。コア30aでは、電気抵抗率が大きい第2磁性層から形成される第2積層部32aおよび第3積層部33bが、第1積層部よりも巻回部21を形成する導線に接近して配置される。   The core 30a has a first laminated portion 31a in which first magnetic layers 41a and insulating layers 51a are alternately laminated, a thickness and a relative magnetic permeability equal to those of the first magnetic layer, and an electric resistivity larger than that of the first magnetic layer. A second laminated portion 32a in which the second magnetic layer 42a and the insulating layer 52a are alternately laminated, and a third laminated portion 33a in which the second magnetic layer 42a and the insulating layer 53a are alternately laminated are provided. Each of the first stacked portion 31a, the second stacked portion 32a, and the third stacked portion 33a (hereinafter, also simply referred to as a stacked portion) has a rectangular parallelepiped shape. The first stacked portion 31a is located on the outermost layer orthogonal to the stacking direction, and is adjacent to the first and second surfaces facing each other, and adjacent to the first and second surfaces, and It is a surface parallel to the direction and the winding axis direction, and has a third surface and a fourth surface facing each other, and two other side surfaces. In the inductor 100, the second laminated portion 32a, the first laminated portion 31a, and the third laminated portion 33a are laminated in this order with the lamination direction being the same to form the core 30a. That is, the second stacked unit 32a and the third stacked unit 33a are arranged on the first and second surfaces of the first stacked unit 31a that face each other so that the stacking directions are parallel. The core 30 a is accommodated in the internal space of the winding part 21 with the laminating direction substantially orthogonal to the winding axis of the winding part 21. In the core 30a, the second laminated portion 32a and the third laminated portion 33b formed from the second magnetic layer having a large electric resistivity are arranged closer to the conductor forming the winding portion 21 than the first laminated portion. You.

図2に示すように、コア30aとコイルの巻回部21が素体40の内部に収容され、コア30aの第2積層部32aおよび第3積層部33aの外側にコイルの巻回部21を構成する導線が近接して配置されている。図2では、コア30aの高さと巻回部21の高さとが略同一に形成されている。コア30aは、第1磁性層41aおよび絶縁層51aが積層されてなる第1積層部31aと、第1磁性層41aより電気抵抗率が大きい第2磁性層42aおよび絶縁層52aが積層されてなる第2積層部32aと、第2磁性層42aおよび絶縁層53aが積層されてなる第3積層部33aとから形成される。第1積層部31a、第2積層部32aおよび第3積層部33aの積層方向は、すべて同一方向となっている。第2積層部32aおよび第3積層部33aの最外層は第2磁性層42aとなっている。また、第2積層部32aおよび第3積層部33aは、第1積層部31aの積層方向の両側の最外層面上にそれぞれ配置され、第1積層部31aよりも巻回部21の導線に近接して配置される。第1積層部31aと、第2積層部32aおよび第3積層部33aとの間にはそれぞれ絶縁層54aおよび55aがそれぞれ配置される。   As shown in FIG. 2, the core 30a and the coil winding portion 21 are housed inside the element body 40, and the coil winding portion 21 is provided outside the second stacked portion 32a and the third stacked portion 33a of the core 30a. The constituent wires are arranged close to each other. In FIG. 2, the height of the core 30a and the height of the winding portion 21 are substantially the same. The core 30a is formed by laminating a first laminated portion 31a in which a first magnetic layer 41a and an insulating layer 51a are laminated, and a second magnetic layer 42a and an insulating layer 52a having a higher electric resistivity than the first magnetic layer 41a. It is formed of a second laminated portion 32a and a third laminated portion 33a in which the second magnetic layer 42a and the insulating layer 53a are laminated. The lamination directions of the first laminated section 31a, the second laminated section 32a, and the third laminated section 33a are all the same. The outermost layer of the second laminated portion 32a and the third laminated portion 33a is the second magnetic layer 42a. Further, the second laminated portion 32a and the third laminated portion 33a are respectively disposed on the outermost layer surfaces on both sides in the laminating direction of the first laminated portion 31a, and are closer to the conductor of the winding portion 21 than the first laminated portion 31a. Placed. Insulating layers 54a and 55a are respectively arranged between the first laminated portion 31a and the second laminated portion 32a and the third laminated portion 33a.

第1磁性層41aおよび第2磁性層42aは、例えば、略同一の厚みで形成され、薄い平板形状を有し、少なくとも電気抵抗率が異なっている。第1磁性層41aおよび第2磁性層42aは、例えば、略同一の比透磁率を有していてもよい。第1磁性層41aおよび第2磁性層42aは、例えば、鉄、ケイ素鋼、パーマロイ、センダスト、パーメンジュール、ソフトフェライト、アモルファス磁性合金、ナノクリスタル磁性合金およびこれらの合金からなる群から選択される軟磁性体である。また第1磁性層41aおよび第2磁性層42aは、素体40を構成する複合材料の比透磁率よりも高い比透磁率を有していれば、他の材料を用いて形成されていてもよい。絶縁層は、第1磁性層41aおよび第2磁性層42aをそれぞれ電気的に絶縁して接着するとともに、積層部間を電気的に絶縁して接着する。図2では、各絶縁層は、略同一の厚みを有している。絶縁層は、例えば、エポキシ樹脂、ポリイミド樹脂およびポリイミドアミド樹脂からなる群から選択される少なくとも1種を含む材料で形成される。   The first magnetic layer 41a and the second magnetic layer 42a are formed, for example, with substantially the same thickness, have a thin plate shape, and have at least different electrical resistivity. The first magnetic layer 41a and the second magnetic layer 42a may have, for example, substantially the same relative magnetic permeability. The first magnetic layer 41a and the second magnetic layer 42a are selected, for example, from the group consisting of iron, silicon steel, permalloy, sendust, permendur, soft ferrite, amorphous magnetic alloy, nanocrystalline magnetic alloy, and alloys thereof. It is a soft magnetic material. The first magnetic layer 41a and the second magnetic layer 42a may be formed using other materials as long as they have a higher relative magnetic permeability than the composite material constituting the element body 40. Good. The insulating layer electrically insulates and bonds the first magnetic layer 41a and the second magnetic layer 42a, and also electrically insulates and bonds between the laminated portions. In FIG. 2, each insulating layer has substantially the same thickness. The insulating layer is formed of, for example, a material containing at least one selected from the group consisting of an epoxy resin, a polyimide resin, and a polyimide amide resin.

第2磁性層42aは、第1磁性層41aよりも大きい電気抵抗率を有している。第2磁性層42aの第1磁性層41aに対する電気抵抗率の比は、例えば、1より大きく、好ましくは1.3以上である。   The second magnetic layer 42a has a higher electrical resistivity than the first magnetic layer 41a. The ratio of the electrical resistivity of the second magnetic layer 42a to the first magnetic layer 41a is, for example, greater than 1, and preferably 1.3 or more.

第1積層部31a、第2積層部32aおよび第3積層部33aの磁性層の厚みaに対する絶縁層の厚みbの厚み比(b/a)は、例えば、0.2以下であり、絶縁層の厚みbは、数μm程度である。ここで厚み比を求める方法の一例を説明する。厚み比(b/a)は、積層部を構成する磁性層の厚みaで、絶縁層の厚みbを除して求められる。厚みaおよび厚みbは、コアの略中央の断面観察画像において積層方向コアの略中心の直線上における全ての磁性層41aおよび42aの厚みと全ての絶縁層51aの厚みをそれぞれの厚みを測定し、その測定値の平均値として求められる。   The thickness ratio (b / a) of the thickness b of the insulating layer to the thickness a of the magnetic layer of each of the first laminated portion 31a, the second laminated portion 32a, and the third laminated portion 33a is, for example, 0.2 or less. Is about several μm. Here, an example of a method for obtaining the thickness ratio will be described. The thickness ratio (b / a) is determined by dividing the thickness b of the insulating layer by the thickness a of the magnetic layer constituting the laminated portion. The thicknesses a and b are measured by measuring the thicknesses of all the magnetic layers 41a and 42a and the thicknesses of all the insulating layers 51a on a straight line substantially at the center of the core in the stacking direction in the cross-sectional observation image at the substantially center of the core. , As an average of the measured values.

一般に、インダクタにおける損失は、コイルを形成する巻線導体に起因する銅損と、コアに起因する渦電流損失とヒステリシス損失の合計である鉄損とに分けられる。また、軽負荷時には、直流重畳電流は小さく、磁束は巻回部を形成する導体に近い位置に集中する。重負荷時には、直流重畳電流は大きく、磁束は導体から遠い位置まで広がる。   Generally, the loss in an inductor is divided into copper loss due to a winding conductor forming a coil and iron loss which is a sum of eddy current loss and hysteresis loss due to a core. When the load is light, the DC superimposed current is small, and the magnetic flux is concentrated at a position near the conductor forming the winding portion. Under heavy load, the DC superimposed current is large, and the magnetic flux spreads far from the conductor.

インダクタ100では、巻回部21の内部空間にコア30aが配置されているので、軽負荷時には、コア30aの巻回部21の導線に近い側の第2積層部32aおよび第3積層部33aにおける渦電流の原因である磁束密度が高くなるが、第2磁性層42aの電気抵抗率が第1磁性層41aよりも大きくなっているため、渦電流損失が低減されて鉄損が小さくなる。一方、重負荷時には、第2積層部32a、第3積層部33aおよび第1積層部31aにおける磁束密度がともに高くなるが、直流重畳電流の増大による銅損がより大きくなるので、鉄損の影響は相対的に小さくなる。したがって、上記の構成を有するインダクタ100では、コアを有しながら、特に軽負荷時における渦電流損失が低減される。   In the inductor 100, since the core 30a is arranged in the internal space of the winding portion 21, the light is applied to the second stacked portion 32a and the third stacked portion 33a on the side closer to the conductor of the winding portion 21 of the core 30a at a light load. Although the magnetic flux density causing the eddy current increases, the electric resistivity of the second magnetic layer 42a is larger than that of the first magnetic layer 41a, so that the eddy current loss is reduced and the iron loss is reduced. On the other hand, at the time of heavy load, the magnetic flux densities in the second laminated portion 32a, the third laminated portion 33a, and the first laminated portion 31a are all high, but the copper loss due to the increase of the DC superimposed current is further increased. Becomes relatively small. Therefore, in the inductor 100 having the above-described configuration, the eddy current loss is reduced particularly at a light load while having the core.

表1に、磁性層bと絶縁層からなる第2積層部、磁性層aと絶縁層からなる第1積層部、および磁性層bと絶縁層からなる第3積層部をこの順に積層したコアを用いた実施例1のインダクタについて、直流重畳電流を0A、交流電流の振幅を10mA、磁性層aの電気抵抗率ρを一定として、磁性層bの電気抵抗率ρを変化させ、インダクタンス値と渦電流損失Peをシミュレーションして求めた結果を示す。実施例1のインダクタでは、磁性層aおよび磁性層bの比透磁率は、それぞれ等しく、磁性層a、bは、飽和磁束密度Bs=1.0Tであり、素体の大きさL×W×Hは、2.0mm×1.6mm×1.0mm、巻線のターン数は8.5とした。また、直流重畳飽和電流は、直流重畳電流が0のインダクタンス値から30%低下した直流重畳電流値とした。なお、シミュレーションは、ムラタソフトウエア社製の有限要素法解析ソフトウエアFemtet(登録商標)を用いて周波数10MHzの調和磁場解析で実施した。
Table 1 shows a core obtained by laminating a second laminated portion including a magnetic layer b and an insulating layer, a first laminated portion including a magnetic layer a and an insulating layer, and a third laminated portion including a magnetic layer b and an insulating layer in this order. With respect to the inductor of Example 1 used, the DC superimposed current was 0 A, the amplitude of the AC current was 10 mA, the electric resistivity ρ a of the magnetic layer a was fixed, and the electric resistivity ρ b of the magnetic layer b was changed. And results obtained by simulating the eddy current loss Pe. In the inductor according to the first embodiment, the relative magnetic permeability of the magnetic layer a and the magnetic layer b are equal to each other, the magnetic layers a and b have the saturation magnetic flux density Bs = 1.0T, and the size of the element body L × W × H was 2.0 mm × 1.6 mm × 1.0 mm, and the number of turns of the winding was 8.5. The DC superimposed saturation current was a DC superimposed current value that was 30% lower than the inductance value of the DC superimposed current of 0. The simulation was performed by a harmonic magnetic field analysis at a frequency of 10 MHz using finite element method analysis software Femtet (registered trademark) manufactured by Murata Software.

Figure 2020053486
Figure 2020053486

実施例1の各インダクタは、インダクタンス値が同一であるから、渦電流損失以外の特性は同じインダクタと見なすことができる。実施例1の結果から、磁性層bの電気抵抗率ρが、磁性層aの電気抵抗率ρよりも大きくなるにしたがい、渦電流損失が低減されていることがわかる。つまり、巻回部に近接して電気抵抗率の高い磁性層を配置することにより、インダクタンス値を維持しつつ、渦電流損失を低減することができる。 Since the inductors of the first embodiment have the same inductance value, it can be considered that the inductors have the same characteristics except for the eddy current loss. The results of Example 1 show that the eddy current loss is reduced as the electric resistivity ρ b of the magnetic layer b becomes larger than the electric resistivity ρ a of the magnetic layer a. In other words, by arranging the magnetic layer having a high electric resistivity close to the winding portion, it is possible to reduce the eddy current loss while maintaining the inductance value.

(実施例2)
実施例2のインダクタは、第2磁性層の比透磁率が、第1磁性層の比透磁率よりも大きいこと以外は、実施例1のインダクタ100と同様に構成される。実施例2のインダクタでは、第2磁性層の電気抵抗率は第1磁性層の電気抵抗率と略同一であってもよい。
(Example 2)
The inductor according to the second embodiment has the same configuration as the inductor 100 according to the first embodiment except that the relative magnetic permeability of the second magnetic layer is larger than the relative magnetic permeability of the first magnetic layer. In the inductor according to the second embodiment, the electrical resistivity of the second magnetic layer may be substantially the same as the electrical resistivity of the first magnetic layer.

表2は、磁性層bと絶縁層からなる第2積層部、磁性層aと絶縁層からなる第1積層部、および磁性層bと絶縁層からなる第3積層部をこの順に積層したコアとなる積層部の構成を変えたインダクタについて、直流重畳電流を0A、交流電流の振幅を10mAとして、磁性層aと磁性層bの厚みと積層数、比透磁率と電気抵抗率を変化させた場合の、インダクタンス値と渦電流損失Peをシミュレーションして求めた結果を示す。実施例2aから2cのインダクタでは、磁性層aおよび磁性層bの厚みは等しく、磁性層bの比透磁率μは磁性層aの比透磁率μより大きくなっており、磁性層aおよび磁性層bの電気抵抗率ρを同様に変化させている。実施例2dから2fのインダクタでは、磁性層aおよび磁性層bの厚みと比透磁率μは、それぞれ等しくなっており、磁性層aおよび磁性層bの電気抵抗率ρを同様に変化させている。 Table 2 shows a core obtained by laminating a second laminated portion including a magnetic layer b and an insulating layer, a first laminated portion including a magnetic layer a and an insulating layer, and a third laminated portion including a magnetic layer b and an insulating layer in this order. When the superposed DC current is 0 A and the amplitude of the AC current is 10 mA, the thickness and the number of layers of the magnetic layers a and b, the relative magnetic permeability and the electric resistivity are changed with respect to an inductor having a different laminated portion configuration. The results obtained by simulating the inductance value and the eddy current loss Pe of FIG. In the inductors of Examples 2a to 2c, the thicknesses of the magnetic layer a and the magnetic layer b are equal, and the relative magnetic permeability μ b of the magnetic layer b is larger than the relative magnetic permeability μ a of the magnetic layer a. The electric resistivity ρ of the magnetic layer b is similarly changed. In the inductors of Examples 2d to 2f, the thickness and relative permeability μ of the magnetic layer a and the magnetic layer b are equal to each other, and the electric resistivity ρ of the magnetic layer a and the magnetic layer b is similarly changed. .

Figure 2020053486
Figure 2020053486

実施例2aから2fは、インダクタンス値に大きな差はないので、渦電流損失以外の特性は同じインダクタと見なすことができる。実施例2aと実施例2d、実施例2bと実施例e、実施例2cと実施例2fをそれぞれ比較すると、磁性層の電気抵抗率が同一の場合には、磁性層bの比透磁率を磁性層aの比透磁率よりも大きくすることで、渦電流損失が低減されていることがわかる。つまり、比透磁率の大きい第2磁性層が積層されてなる第2積層部および第3積層部が巻回部に近接して配置されることにより、特に軽負荷時における渦電流損失が低減される。   In Examples 2a to 2f, there is no significant difference in the inductance value, so that the characteristics other than the eddy current loss can be regarded as the same inductor. Comparing Example 2a and Example 2d, Example 2b and Example e, and Example 2c and Example 2f, when the electrical resistivity of the magnetic layer is the same, the relative permeability of the magnetic layer b is changed to the magnetic permeability. It can be seen that the eddy current loss is reduced by increasing the relative magnetic permeability of the layer a. That is, since the second laminated portion and the third laminated portion in which the second magnetic layer having a large relative magnetic permeability is laminated are disposed close to the winding portion, eddy current loss particularly at a light load is reduced. You.

ここで、インダクタの渦電流損失について説明する。
一般にインダクタにおいて、磁性層と絶縁層を積層して形成されるコアの磁性層における渦電流損失Peは、磁性層の厚みtが平板状の磁性層の面方向の幅よりも充分に小さい場合、磁性層の電気抵抗率をρ、比透磁率をμとすると、厚みtの二乗に比例し、電気抵抗率ρと比透磁率μの積の平方根に反比例する。すなわち渦電流損失Peは下式(1)で表される。

Figure 2020053486
Here, the eddy current loss of the inductor will be described.
In general, in the inductor, the eddy current loss Pe in the magnetic layer of the core formed by laminating the magnetic layer and the insulating layer is such that when the thickness t of the magnetic layer is sufficiently smaller than the width in the surface direction of the flat magnetic layer, Assuming that the electrical resistivity of the magnetic layer is ρ and the relative magnetic permeability is μ, it is proportional to the square of the thickness t and inversely proportional to the square root of the product of the electrical resistivity ρ and the relative magnetic permeability μ. That is, the eddy current loss Pe is expressed by the following equation (1).
Figure 2020053486

例えば、実施例1のインダクタ100では、第2積層部および第3積層部で生じる渦電流損失を第1積層部で生じる渦電流損失より小さくするために、第2積層部および第3積層部の磁性層の電気抵抗率のみを大きくした。しかし、式(1)から、第2積層部および第3積層部で生じる渦電流損失を第1積層部で生じる渦電流損失より小さくするには、第2磁性層の厚みの二乗を第2磁性層の比透磁率と電気抵抗率の積の平方根で除した数値が、第1磁性層の厚みの二乗を第1磁性層の比透磁率と電気抵抗率の積の平方根で除した数値よりも小さくすれよいことがわかる。すなわち、第2磁性層の電気抵抗率を第1磁性層の電気抵抗率より大きくすることに加えて、それぞれの磁性層の比透磁率を変更することによって、渦電流損失をより小さくすることができる。   For example, in the inductor 100 according to the first embodiment, the eddy current loss generated in the second stacked portion and the third stacked portion is made smaller than the eddy current loss generated in the first stacked portion. Only the electric resistivity of the magnetic layer was increased. However, from the equation (1), in order to make the eddy current loss generated in the second and third stacked portions smaller than the eddy current loss generated in the first stacked portion, the square of the thickness of the second magnetic layer must be equal to the second magnetic layer. The value obtained by dividing the square of the thickness of the first magnetic layer by the square root of the product of the relative permeability of the first magnetic layer and the electrical resistivity is smaller than the value obtained by dividing the square root of the product of the relative magnetic permeability and the electrical resistivity of the layer. It turns out that it is good to be small. That is, in addition to making the electric resistivity of the second magnetic layer larger than the electric resistivity of the first magnetic layer, it is possible to further reduce the eddy current loss by changing the relative permeability of each magnetic layer. it can.

(実施例3)
実施例3のインダクタは、第2磁性層の電気抵抗率と比透磁率の積が、第1磁性層の電気抵抗率と比透磁率の積よりも大きいという関係を満たすこと以外は、実施例1のインダクタ100と同様に構成される。第1磁性層と第2磁性層は、厚みおよび比透磁率が等しい。実施例3のインダクタでは、第1磁性層および第2磁性層の電気抵抗率および比透磁率がそれぞれ異なっていてもよく、第1磁性層および第2磁性層の電気抵抗率が略同一で、比透磁率が異なっていてもよく、第1磁性層および第2磁性層の比透磁率が略同一で、電気抵抗率が異なっていてもよい。
(Example 3)
The inductor according to the third embodiment is different from the inductor according to the third embodiment except that the product of the electrical resistivity of the second magnetic layer and the relative magnetic permeability is larger than the product of the electrical resistivity of the first magnetic layer and the relative magnetic permeability. The configuration is the same as that of the first inductor 100. The first magnetic layer and the second magnetic layer have the same thickness and the same relative magnetic permeability. In the inductor of the third embodiment, the first magnetic layer and the second magnetic layer may have different electrical resistivity and relative magnetic permeability, and the first magnetic layer and the second magnetic layer have substantially the same electrical resistivity. The relative magnetic permeability may be different, the first magnetic layer and the second magnetic layer may have substantially the same relative magnetic permeability, and may have different electrical resistivity.

実施例3のインダクタでは、電気抵抗率と比透磁率の積が第1磁性層よりも大きい第2磁性層が積層されてなる第2積層部および第3積層部が、巻回部の導体に近接して配置されるため、特に軽負荷時における渦電流損失が低減される。   In the inductor according to the third embodiment, the second laminated portion and the third laminated portion in which the second magnetic layer having the product of the electric resistivity and the relative magnetic permeability is larger than the first magnetic layer are laminated on the conductor of the winding portion. Since they are arranged close to each other, eddy current loss particularly at light load is reduced.

(実施例4)
実施例4のインダクタが内蔵するコア30fの構成を、図3を参照して説明する。コア30fでは、第1積層部31fを構成する第1磁性層41fの厚みと、第2積層部32fおよび第3積層部33fを構成する第2磁性層42fの厚みとが異なっていること以外は、実施例1のインダクタ100、実施例2のインダクタまたは実施例3のインダクタと同様に構成される。
(Example 4)
The configuration of the core 30f included in the inductor of the fourth embodiment will be described with reference to FIG. In the core 30f, except that the thickness of the first magnetic layer 41f constituting the first laminated portion 31f is different from the thickness of the second magnetic layer 42f constituting the second laminated portion 32f and the third laminated portion 33f. , The inductor 100 of the first embodiment, the inductor of the second embodiment, or the inductor of the third embodiment.

コア30fでは、第1積層部31fが、第1磁性層41fと絶縁層51fとが素体の長手方向Lとコイルの巻軸方向Zに直交するW方向に積層されて形成されている。
第2積層部32fは、第2磁性層42fと絶縁層52fとが素体の短手方向Wに積層され、第3積層部33fは、第2磁性層42fと絶縁層53fとが素体の短手方向W方向に積層されて形成されている。第2積層部32fおよび第3積層部33fは、第1積層部31fの積層方向の両側の最外層面上に絶縁層54fおよび55fを介してそれぞれ配置される。コア30fでは、第2磁性層42fの厚みは、第1磁性層41fの厚みよりも薄く形成され、第2磁性層42fの厚みの二乗を第2磁性層42fの比透磁率と電気抵抗率の積の平方根で除した数値が、第1磁性層41fの厚みの二乗を第1磁性層41fの比透磁率と電気抵抗率の積の平方根で除した数値よりも小さくなっている。これにより、より効果的に軽負荷時における渦電流損失を低減することができる。
In the core 30f, the first laminated portion 31f is formed by laminating the first magnetic layer 41f and the insulating layer 51f in the W direction orthogonal to the longitudinal direction L of the element body and the winding axis direction Z of the coil.
The second laminated portion 32f is configured such that the second magnetic layer 42f and the insulating layer 52f are laminated in the lateral direction W of the element body, and the third laminated portion 33f is configured such that the second magnetic layer 42f and the insulating layer 53f are composed of the element body. It is formed by being laminated in the short direction W direction. The second laminated portion 32f and the third laminated portion 33f are arranged on the outermost layer surfaces on both sides in the laminating direction of the first laminated portion 31f via insulating layers 54f and 55f, respectively. In the core 30f, the thickness of the second magnetic layer 42f is formed to be thinner than the thickness of the first magnetic layer 41f, and the square of the thickness of the second magnetic layer 42f is calculated as the square of the relative magnetic permeability and electric resistivity of the second magnetic layer 42f. The value divided by the square root of the product is smaller than the value obtained by dividing the square of the thickness of the first magnetic layer 41f by the square root of the product of the relative magnetic permeability and the electric resistivity of the first magnetic layer 41f. Thereby, the eddy current loss at the time of light load can be reduced more effectively.

(実施例5)
実施例4のインダクタ110を、図4を参照して説明する。図4は、図1のA−Aと同じ位置におけるインダクタ110の概略断面図である。インダクタ110は、コア30bにおいて、巻回部21のコイルの端部が引き出される側21aに近接して配置される第3積層部33bにおける第2磁性層42aの積層数が、第2積層部32bにおける積層数よりも多くなっていること以外は、実施例1のインダクタ100、実施例2のインダクタまたは実施例3のインダクタと同様に構成される。
(Example 5)
Fourth Embodiment An inductor 110 according to a fourth embodiment will be described with reference to FIG. FIG. 4 is a schematic sectional view of the inductor 110 at the same position as AA in FIG. In the inductor 110, in the core 30b, the number of laminations of the second magnetic layer 42a in the third laminated portion 33b disposed close to the side 21a from which the end of the coil of the wound portion 21 is drawn out is the second laminated portion 32b The configuration is the same as that of the inductor 100 of the first embodiment, the inductor of the second embodiment, or the inductor of the third embodiment, except that the number of layers is larger than the number of layers in.

1対の引き出し部が、素体の互いに対向する端面に向けて引き出される場合、端面に平行な断面において、巻回部は左右対称ではない。つまり、図4の断面図において、引き出し部が巻回部21の右側21aから引き出される場合、巻回部21の右側21aの方が、巻回部21の左側21bよりも、導線が1ターン分多く巻回されることになる。これにより、巻回部21の右側21aの方が巻回部21の左側21bと比較して磁束密度が高くなる。インダクタ110では、第2磁性層42aの積層数が第2積層部32bと第3積層部33bとでは異なり、巻回部21の右側21aに配置される第3積層部33bにおける積層数の方が多くなっている。この構成により、軽負荷時においてインダクタ110に発生する損失をより効果的に低減することができる。なお、コイルの引き出し部は、対向する端面方向に引き出されたのち、対向する端面に露出させてもよく、曲げられて素体の底面に露出させてもよい。   When the pair of drawers are drawn toward the end faces of the element body facing each other, the winding portions are not bilaterally symmetric in a cross section parallel to the end faces. That is, in the cross-sectional view of FIG. 4, when the lead portion is pulled out from the right side 21 a of the winding portion 21, the right side 21 a of the winding portion 21 is one turn longer than the left side 21 b of the winding portion 21. It will be wound many times. As a result, the right side 21a of the winding portion 21 has a higher magnetic flux density than the left side 21b of the winding portion 21. In the inductor 110, the number of laminations of the second magnetic layer 42a is different between the second lamination 32b and the third lamination 33b, and the number of laminations in the third lamination 33b disposed on the right side 21a of the winding part 21 is larger. More. With this configuration, it is possible to more effectively reduce the loss that occurs in inductor 110 at a light load. Note that, after being pulled out in the direction of the facing end surface, the lead portion of the coil may be exposed on the facing end surface, or may be bent and exposed on the bottom surface of the element body.

(実施例6)
実施例6のインダクタが内蔵するコア30cの構成を、図5を参照して説明する。実施例6のインダクタでは、コア30cにおける第1積層部31cの積層方向と、第2積層部32cおよび第3積層部33cの積層方向とが略直交している点が、実施例1のインダクタ100、実施例2のインダクタまたは実施例3のインダクタと異なり、それ以外は実施例1のインダクタ100、実施例2のインダクタまたは実施例3のインダクタと同様に構成される。
(Example 6)
The configuration of the core 30c included in the inductor of the sixth embodiment will be described with reference to FIG. In the inductor according to the sixth embodiment, the point that the stacking direction of the first stacked portion 31c in the core 30c and the stacking direction of the second stacked portion 32c and the third stacked portion 33c are substantially orthogonal to each other is different from the inductor 100 according to the first embodiment. Unlike the inductor of the second embodiment or the inductor of the third embodiment, the other configuration is the same as that of the inductor 100 of the first embodiment, the inductor of the second embodiment, or the inductor of the third embodiment.

コア30cでは、第1積層部31cが、第1磁性層41cと絶縁層51cとが素体の短手方向Wに積層されて形成されている。第2積層部32cは、第2磁性層42cと絶縁層52cとが、素体の長手方向Lに積層され、第3積層部33cは、第2磁性層42cと絶縁層53cとが素体の長手方向Lに積層されて形成されている。第2積層部32cおよび第3積層部33cは、第1積層部31cの積層方向の両側の最外層面上に絶縁層54cおよび55cを介して配置され、第1積層部31cの積層方向の両側の最外装面を被覆している。第2積層部32cおよび第3積層部33cにおける第2磁性層42cの積層数は、実施例1のコア30aの、第2積層部32aおよび第3積層部33aにおける第2磁性層42aの積層数よりも多くなっているが、磁路に直交する磁性層の幅(W方向)も小さくなっている。渦電流損失は、磁路に直交する磁性層の幅(W方向)にも比例するので、そのため、軽負荷時におけるインダクタの渦電流損失がさらに低減される。   In the core 30c, the first laminated portion 31c is formed by laminating the first magnetic layer 41c and the insulating layer 51c in the lateral direction W of the element body. In the second laminated portion 32c, the second magnetic layer 42c and the insulating layer 52c are laminated in the longitudinal direction L of the body, and in the third laminated portion 33c, the second magnetic layer 42c and the insulating layer 53c are formed of the body. It is formed by being laminated in the longitudinal direction L. The second laminated portion 32c and the third laminated portion 33c are disposed on the outermost layer surfaces on both sides of the first laminated portion 31c in the laminating direction via insulating layers 54c and 55c, and are disposed on both sides of the first laminated portion 31c in the laminating direction. Covers the outermost surface. The number of laminations of the second magnetic layer 42c in the second lamination 32c and the third lamination 33c is the number of laminations of the second magnetic layer 42a in the second lamination 32a and the third lamination 33a of the core 30a of the first embodiment. However, the width (W direction) of the magnetic layer perpendicular to the magnetic path is also smaller. Since the eddy current loss is also proportional to the width (W direction) of the magnetic layer orthogonal to the magnetic path, the eddy current loss of the inductor at light load is further reduced.

(実施例7)
実施例7のインダクタが内蔵するコア30dの構成を、図6を参照して説明する。実施例7のインダクタでは、コア30dにおける第1積層部31dの積層方向が、素体の長手方向Lに略平行であり、第2積層部および第3積層部の積層方向と直交していること以外は、実施例1のインダクタ100、実施例2のインダクタまたは実施例3のインダクタと同様に構成される。
(Example 7)
A configuration of a core 30d included in the inductor of the seventh embodiment will be described with reference to FIG. In the inductor according to the seventh embodiment, the stacking direction of the first stacked portion 31d in the core 30d is substantially parallel to the longitudinal direction L of the element body, and is orthogonal to the stacking direction of the second stacked portion and the third stacked portion. Except for this point, the configuration is the same as that of the inductor 100 of the first embodiment, the inductor of the second embodiment, or the inductor of the third embodiment.

コア30dでは、第1積層部31dが、第1磁性層41dと絶縁層51dとが素体の長手方向Lに積層されて形成されている。第2積層部32dは、第2磁性層42dと絶縁層52dとが、素体の短手方向Wに積層されて形成され、第3積層部33dは、第2磁性層42dと絶縁層53dとがそれぞれ素体の短手方向Wに積層されて形成されている。第2積層部32dおよび第3積層部33dは、第1積層部31dの積層方向の両側の最外層面上に隣接し、巻軸方向に平行な面であって、互いに対向する側面である第3の面および第4の面上に、絶縁層54dおよび55dを介して配置され、第1積層部31dの対向する側面を被覆している。
第1積層部31dにおける第1磁性層41dの積層数は、実施例1のコア30aの、第1積層部31aの積層数より多くなっているが、磁路に直交する磁性層の幅(W方向)は小さくなっている。そのため、長手方向Lの対向する端面で生じる渦電流損失を低減してすることができ、軽負荷時におけるインダクタの損失が低減される。
In the core 30d, the first laminated portion 31d is formed by laminating the first magnetic layer 41d and the insulating layer 51d in the longitudinal direction L of the element body. The second laminated portion 32d is formed by laminating a second magnetic layer 42d and an insulating layer 52d in the lateral direction W of the element body. Are laminated in the lateral direction W of the element body. The second stacked portion 32d and the third stacked portion 33d are adjacent to the outermost layer surfaces on both sides in the stacking direction of the first stacked portion 31d, are surfaces parallel to the winding axis direction, and are side surfaces facing each other. On the third and fourth surfaces, insulating layers 54d and 55d are interposed to cover the opposing side surfaces of the first laminated portion 31d.
The number of stacked first magnetic layers 41d in the first stacked portion 31d is larger than the number of stacked first stacked portions 31a of the core 30a of the first embodiment, but the width of the magnetic layer orthogonal to the magnetic path (W Direction) is smaller. Therefore, the eddy current loss generated at the end faces facing each other in the longitudinal direction L can be reduced, and the loss of the inductor at light load is reduced.

(実施例8)
実施例8のインダクタが内蔵するコア30eの構成を、図7を参照して説明する。コア30eでは、第2積層部32eおよび第3積層部33eがそれぞれ、巻軸方向Zに略直交するギャップ部44eおよび45eでそれぞれ分割されていること以外は、実施例1のインダクタ100、実施例2のインダクタまたは実施例3のインダクタと同様に構成される。
(Example 8)
The configuration of the core 30e included in the inductor of the eighth embodiment will be described with reference to FIG. In the core 30e, except that the second laminated portion 32e and the third laminated portion 33e are respectively divided by gap portions 44e and 45e substantially orthogonal to the winding axis direction Z, the inductor 100 of the first embodiment and the third embodiment are different from each other. The configuration is the same as that of the second inductor or the third embodiment.

コア30eでは、第1積層部31eが、第1磁性層41eと絶縁層51eとが素体の短手方向Wに積層されて形成されている。第2積層部32eは、第2磁性層42eと絶縁層52eとが素体の短手方向Wに積層され、第3積層部33eは、第2磁性層42eと絶縁層53eとが素体の短手方向Wに積層されて形成される。第2積層部32eおよび第3積層部33eは、第1積層部31eの積層方向の両側の最外層面上に、絶縁層54eおよび55eを介して配置される。さらに、第2積層部32eは、巻軸方向Zに直交するギャップ部44eで分割され、第3積層部33eは、巻軸方向Zに直交するギャップ部45eで分割されている。ギャップ部44eおよび45eは、第2積層部32eおよび第3積層部33eのそれぞれにおいて外周部まで延在し、第2積層部32eおよび第3積層部33eの側面および積層方向の両側の最外層面から露出している。ギャップ部44eおよび45eは、分割された第2積層部32eおよび第3積層部33eをそれぞれ接着する材料で形成される。また、ギャップ部44eおよび45eは、第2磁性層42eよりも比透磁率が低い材料で形成される。さらにギャップ部44eおよび45eの比透磁率は素体の比透磁率よりも低くてもよく、非磁性材料であってもよい。   In the core 30e, the first laminated portion 31e is formed by laminating the first magnetic layer 41e and the insulating layer 51e in the lateral direction W of the element body. The second laminated portion 32e is formed by laminating the second magnetic layer 42e and the insulating layer 52e in the lateral direction W of the body, and the third laminated portion 33e is formed by combining the second magnetic layer 42e and the insulating layer 53e with the body. It is formed by being laminated in the short direction W. The second stacked unit 32e and the third stacked unit 33e are disposed on the outermost layer surfaces on both sides in the stacking direction of the first stacked unit 31e via insulating layers 54e and 55e. Further, the second stacked portion 32e is divided by a gap portion 44e orthogonal to the winding axis direction Z, and the third stacked portion 33e is split by a gap portion 45e orthogonal to the winding axis direction Z. The gap portions 44e and 45e extend to the outer peripheral portion in each of the second stacked portion 32e and the third stacked portion 33e, and the side surfaces of the second stacked portion 32e and the third stacked portion 33e and the outermost layer surfaces on both sides in the stacking direction. It is exposed from. The gap portions 44e and 45e are formed of a material that bonds the divided second laminated portion 32e and third laminated portion 33e, respectively. The gaps 44e and 45e are formed of a material having a lower relative magnetic permeability than the second magnetic layer 42e. Further, the relative magnetic permeability of the gap portions 44e and 45e may be lower than the relative magnetic permeability of the element body, or may be a non-magnetic material.

第2積層部32eおよび第3積層部33eでは、ギャップ部44eおよび45eが巻軸方向Zに直交して磁気ギャップとして機能して、巻軸方向における磁気抵抗が高くなる。これにより渦電流損失がより低減される。   In the second laminated portion 32e and the third laminated portion 33e, the gap portions 44e and 45e function as magnetic gaps orthogonal to the winding axis direction Z, and the magnetic resistance in the winding axis direction is increased. Thereby, the eddy current loss is further reduced.

インダクタ100では、コイルを形成する導体は平角線であるが、断面が略円形状、多角形状の導体であってもよい。
インダクタ100では、コイルの巻回部の巻軸方向からみた外形形状は、楕円または長円形状であるが、円形状、矩形状、多角形状等であってもよい。コイルの巻回部は、導線が2段に巻回された、いわゆるα巻線形状(例えば、特開2009−239076号公報参照)で形成されているが、エッジワイズ巻、めっき導体パターン等で形成されていてもよい。
インダクタ100では、コイルの両端部が素体の端面方向にそれぞれ引き出されているが、素体の側面方向にそれぞれ引き出されていてもよい。
インダクタ100では、コアの高さと巻回部の高さとが略同一に形成されているが、コアの高さが、巻回部の高さより高くてもよく、また低くてもよい。
インダクタ100では、第1磁性層および第2磁性層は、厚みが異なっていてもよい。
実施例8のコア30eでは、ギャップ部は第2積層部および第3積層部に設けられるが、第1積層部にギャップ部を設けてもよく、第2積層部および第3積層部のいずれか一方のみにギャップ部が設けられていてもよい。
実施例6または実施例7のインダクタでは、第1積層部、第2積層部および第3積層部の少なくとも1つに実施例8のコア30eと同様にギャップ部が設けられてもよい。
実施例1から8のインダクタでは、コアは直方体形状であるが、コアの辺の少なくとも1つが平面または曲面で除去されていてもよい。
コアは、第2積層部、第1積層部および第3積層部をこの順に積層したが、第2積層部または第3積層部のどちらか一方のみでもよい。
In the inductor 100, the conductor forming the coil is a rectangular wire, but may be a conductor having a substantially circular or polygonal cross section.
In the inductor 100, the outer shape of the winding portion of the coil as viewed from the winding axis direction is an ellipse or an ellipse, but may be a circle, a rectangle, a polygon, or the like. The winding portion of the coil is formed in a so-called α-winding shape (for example, see Japanese Patent Application Laid-Open No. 2009-239076) in which a conductive wire is wound in two steps, and is formed by an edgewise winding, a plated conductor pattern, or the like. It may be formed.
In the inductor 100, both ends of the coil are drawn out in the direction of the end face of the body, but may be drawn out in the side direction of the body.
In the inductor 100, the height of the core and the height of the winding portion are substantially the same, but the height of the core may be higher or lower than the height of the winding portion.
In the inductor 100, the first magnetic layer and the second magnetic layer may have different thicknesses.
In the core 30e according to the eighth embodiment, the gap portion is provided in the second stacked portion and the third stacked portion. However, the gap portion may be provided in the first stacked portion, and any one of the second stacked portion and the third stacked portion may be provided. A gap may be provided only on one side.
In the inductor according to the sixth or seventh embodiment, a gap may be provided in at least one of the first, second, and third stacked units, similarly to the core 30e according to the eighth embodiment.
In the inductors of the first to eighth embodiments, the core has a rectangular parallelepiped shape, but at least one of the sides of the core may be removed by a flat surface or a curved surface.
Although the core has the second laminated portion, the first laminated portion, and the third laminated portion laminated in this order, it may be only one of the second laminated portion and the third laminated portion.

20 コイル
21 巻回部
22a、22b 引き出し部
30a、30b、30c、30d、30e コア
31a、32a、33a 31b、32b、33b、31c、32c、33c、31d、32d、33d、31e、32e、33e、31f、32f、33f 積層部
40 素体
41a、42a、41c、42c、41d、42d、41e、42e、41f、42f 磁性層
44e、45e ギャップ部
51a、52a、53a、54a、55a 絶縁層
60 外部端子
100、110 インダクタ
20 Coil 21 Winding part 22a, 22b Pull-out part 30a, 30b, 30c, 30d, 30e Core 31a, 32a, 33a 31b, 32b, 33b, 31c, 32c, 33c, 31d, 32d, 33d, 31e, 32e, 33e, 31f, 32f, 33f Laminated part 40 Element body 41a, 42a, 41c, 42c, 41d, 42d, 41e, 42e, 41f, 42f Magnetic layer 44e, 45e Gap part 51a, 52a, 53a, 54a, 55a Insulating layer 60 External terminal 100, 110 inductor

Claims (7)

磁性層と絶縁層とが交互に積層される積層部を含むコアと、
前記コアの周囲に巻回される巻回部と巻回部から引き出される1対の引き出し部を含み、前記巻回部の巻軸が前記積層部の積層方向と略直交して配置されるコイルと、
対向する端面を有し、前記コアおよび前記コイルを収容する素体と、
を備え、
前記磁性層は、第1磁性層と、前記第1磁性層よりも電気抵抗率が大きい第2磁性層とを含み、
前記積層部は、前記第1磁性層および絶縁層が交互に積層される第1積層部と、前記第2磁性層および絶縁層が交互に積層される第2積層部および第3積層部とを含み、
前記第1積層部は、積層方向に直交し、互いに対向する第1の面および第2の面と、積層方向および巻軸方向に平行な面であり、互いに対向する第3の面および第4の面とを有し、
前記第2積層部は前記第1の面に配置され、前記第3積層部は前記第2の面に配置されるか、または
前記第2積層部は前記第3の面に配置され、前記第3積層部は前記第4の面に配置されるインダクタ。
A core including a laminated portion in which a magnetic layer and an insulating layer are alternately laminated,
A coil including a wound portion wound around the core and a pair of drawn portions pulled out from the wound portion, wherein a winding axis of the wound portion is disposed substantially orthogonal to a stacking direction of the stacked portion; When,
A body having opposing end faces and housing the core and the coil;
With
The magnetic layer includes a first magnetic layer and a second magnetic layer having a higher electric resistivity than the first magnetic layer,
The laminated portion includes a first laminated portion in which the first magnetic layer and the insulating layer are alternately laminated, and a second laminated portion and a third laminated portion in which the second magnetic layer and the insulating layer are alternately laminated. Including
The first laminated portion is a first surface and a second surface orthogonal to the laminating direction and opposed to each other, and a third surface and a fourth surface parallel to the laminated direction and the winding axis direction. With the surface of
The second laminated portion is disposed on the first surface, the third laminated portion is disposed on the second surface, or the second laminated portion is disposed on the third surface, and the second laminated portion is disposed on the third surface. The three stacked portions are inductors arranged on the fourth surface.
磁性層と絶縁層とが交互に積層される積層部を含むコアと、
前記コアの周囲に巻回される巻回部と巻回部から引き出される1対の引き出し部を含み、前記巻回部の巻軸が前記積層部の積層方向と略直交して配置されるコイルと、
対向する端面を有し、前記コアおよび前記コイルを収容する素体と、
を備え、
前記磁性層は、第1磁性層と、前記第1磁性層よりも比透磁率が大きい第2磁性層とを含み、
前記積層部は、前記第1磁性層および絶縁層が交互に積層される第1積層部と、前記第2磁性層および絶縁層が交互に積層される第2積層部および第3積層部とを含み、
前記第1積層部は、積層方向に直交し、互いに対向する第1の面および第2の面と、積層方向および巻軸方向に平行な面であり、互いに対向する第3の面および第4の面とを有し、
前記第2積層部は前記第1の面に配置され、前記第3積層部は前記第2の面に配置されるか、または
前記第2積層部は前記第3の面に配置され、前記第3積層部は前記第4の面に配置されるインダクタ。
A core including a laminated portion in which a magnetic layer and an insulating layer are alternately laminated,
A coil including a wound portion wound around the core and a pair of drawn portions pulled out from the wound portion, wherein a winding axis of the wound portion is disposed substantially orthogonal to a stacking direction of the stacked portion; When,
A body having opposing end faces and housing the core and the coil;
With
The magnetic layer includes a first magnetic layer and a second magnetic layer having a higher relative magnetic permeability than the first magnetic layer,
The laminated portion includes a first laminated portion in which the first magnetic layer and the insulating layer are alternately laminated, and a second laminated portion and a third laminated portion in which the second magnetic layer and the insulating layer are alternately laminated. Including
The first laminated portion is a first surface and a second surface orthogonal to the laminating direction and opposed to each other, and a third surface and a fourth surface parallel to the laminated direction and the winding axis direction. With the surface of
The second laminated portion is disposed on the first surface, the third laminated portion is disposed on the second surface, or the second laminated portion is disposed on the third surface, and the second laminated portion is disposed on the third surface. The three stacked portions are inductors arranged on the fourth surface.
前記第2磁性層の電気抵抗率と比透磁率との積は、前記第1磁性層の電気抵抗率と比透磁率との積よりも大きい請求項1または請求項2に記載のインダクタ。   3. The inductor according to claim 1, wherein a product of an electric resistivity of the second magnetic layer and a relative magnetic permeability is larger than a product of an electric resistivity of the first magnetic layer and a relative magnetic permeability. 前記1対の引き出し部は、前記巻回部の外周から前記素体の対向する端面方向にそれぞれ引き出され、
前記第2積層部における第2磁性層の積層数と、前記第3積層部における第2磁性層の積層数とが異なる請求項1から請求項3のいずれかに記載のインダクタ。
The pair of pull-out portions are pulled out from the outer periphery of the winding portion in the direction of opposed end faces of the body, respectively,
4. The inductor according to claim 1, wherein the number of laminated second magnetic layers in the second laminated portion is different from the number of laminated second magnetic layers in the third laminated portion. 5.
前記第1積層部、第2積層部および第3積層部のうち、少なくとも2つの積層方向が異なる請求項1から請求項4のいずれかに記載のインダクタ。   5. The inductor according to claim 1, wherein at least two of the first, second, and third laminated portions have different laminating directions. 6. 前記第1積層部、第2積層部および第3積層部のうち、少なくとも1つは前記巻回部の巻軸方向に略直交する少なくとも1つの面で分割されている請求項1から請求項5のいずれかに記載のインダクタ。   The at least one of the first laminated portion, the second laminated portion, and the third laminated portion is divided by at least one surface substantially orthogonal to a winding axis direction of the winding portion. The inductor according to any one of the above. 前記コアは、前記第2磁性層の厚みの二乗を前記第2磁性層の比透磁率と電気抵抗率の積の平方根で除した数値が、
前記第1磁性層の厚みの二乗を前記第1磁性層の比透磁率と電気抵抗率の積の平方根で除した数値よりも小さい請求項1から請求項6のいずれかに記載のインダクタ。
The core has a value obtained by dividing the square of the thickness of the second magnetic layer by the square root of the product of the relative magnetic permeability and the electric resistivity of the second magnetic layer,
The inductor according to any one of claims 1 to 6, wherein the square of the thickness of the first magnetic layer is smaller than a value obtained by dividing the square of the product of the relative magnetic permeability and the electrical resistivity of the first magnetic layer.
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Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH04106910A (en) * 1990-08-27 1992-04-08 Tdk Corp Electronic parts
JP2016195245A (en) * 2015-04-01 2016-11-17 サムソン エレクトロ−メカニックス カンパニーリミテッド. Coil electronic component and method for manufacturing the same
JP2016219781A (en) * 2015-05-19 2016-12-22 サムソン エレクトロ−メカニックス カンパニーリミテッド. Coil electronic component and method of manufacturing the same
WO2017065528A1 (en) * 2015-10-16 2017-04-20 주식회사 모다이노칩 Power inductor
WO2018079402A1 (en) * 2016-10-31 2018-05-03 株式会社村田製作所 Inductor

Family Cites Families (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6417753B1 (en) * 2000-02-17 2002-07-09 Koninklijke Philips Electronics N.V. Planar magnetic device without center core leg
CN100517526C (en) * 2002-10-31 2009-07-22 松下电器产业株式会社 Inductance part and electronic device using the same
US7375608B2 (en) * 2003-09-29 2008-05-20 Tamura Corporation Solid electrolytic capacitor and manufacturing method thereof
JP2016119385A (en) 2014-12-20 2016-06-30 東光株式会社 Surface mounting inductor and method of manufacturing the same
JP6757622B2 (en) * 2016-08-10 2020-09-23 株式会社村田製作所 Electronic components
KR20180022153A (en) * 2016-08-23 2018-03-06 삼성전기주식회사 Common mode filter and manufacturing method of the same
US10525690B2 (en) * 2016-09-07 2020-01-07 General Electric Company Additive manufacturing-based low-profile inductor

Patent Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH04106910A (en) * 1990-08-27 1992-04-08 Tdk Corp Electronic parts
JP2016195245A (en) * 2015-04-01 2016-11-17 サムソン エレクトロ−メカニックス カンパニーリミテッド. Coil electronic component and method for manufacturing the same
JP2016219781A (en) * 2015-05-19 2016-12-22 サムソン エレクトロ−メカニックス カンパニーリミテッド. Coil electronic component and method of manufacturing the same
WO2017065528A1 (en) * 2015-10-16 2017-04-20 주식회사 모다이노칩 Power inductor
WO2018079402A1 (en) * 2016-10-31 2018-05-03 株式会社村田製作所 Inductor

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